Axial buckling behavior of perfect and defective zigzag single-walled carbon nanotubes (SWCNTs) is
studied by molecular dynamics (MD) simulations. Different effects of three typical categories of defect on the
axial buckling properties of SWCNTs are investigated. MD simulation results show that the buckling behavior of
defective tubes is quite different from the perfect tube. The critical buckling load of zigzag SWCNTs is significantly
reduced with different defect appeared in the tube wall, and the effective elastic modulus are also slightly but
distinguishingly influenced by individual defect. It is revealed that an Stone-Thrower-Wales defect could induce
greater decrease of the rigidity a single vacancy defect or a double vacancies one. The harmful effects of defects
do not depend simply on the size of the defective area, but related strongly to the buckling modes of the defective
SWCNTs which specifically differ from each other due to the different defect structures.
XIN Hao1 (辛浩), HAN Qiang2,3* (韩强)
. Mechanical Properties of Perfect and Defective Zigzag Single-Walled
Carbon Nanotubes Under Axial Compression[J]. Journal of Shanghai Jiaotong University(Science), 2012
, 17(5)
: 545
-551
.
DOI: 10.1007/s12204-012-1323-8
[1] Krishnan A, Dujardin E, Ebbesen T W, et al.Young’s modulus of single-walled nanotubes [J]. Physical Review B, 1998, 58(20): 14013-14019.
[2] Lu J P. Elastic properties of carbon nanotubes and nanoropes [J]. Physical Review Letters, 1997, 79(7):1297-1300.
[3] Hashimoto A, Suenaga K, Gloter A, et al. Direct evidence for atomic defects in graphene layers [J].Nature, 2004, 430(7002): 870-873.
[4] Chowdhury S C, Okabe T. Computer simulation of carbon nanotube pull-out from polymer by the molecular dynamics method [J]. Composites. Part A: Applied Science and Manufacturing, 2007, 38(3): 747-754.
[5] Xin H, Han Q, Yao X H. Buckling and axially compressive properties of perfect and defective singlewalled carbon nanotubes [J]. Carbon, 2007, 45(13):2486-2495.
[6] Xin H, Han Q, Yao X H. Buckling of defective singlewalled and double-walled carbon nanotubes under axial compression by molecular dynamics simulation [J].Composites Science and Technology, 2008, 68(7-8):1809-1814.
[7] Xin H, Han Q. The strain rate effect of perfect and defective single-walled carbon nanotubes under axial compression [J]. Journal of Computational and Theoretical Nanoscience, 2012, 9(3): 371-378.
[8] Brenner D W. Empirical potential for hydrocarbons for use in simulating the chemical vapor deposition of diamond films [J]. Physical Review B, 1990, 42(15):9458-9471.
[9] Mayo S L, Olafson B D, GoddardW A III. Dreiding:a generic force field for molecular simulations [J].Journal of Physical Chemistry, 1990, 94(26): 8897-8909.
[10] Sears A, Batra R C. Macroscopic properties of carbon nanotubes from molecular- mechanics simulations [J]. Physical Review B, 2004, 69(23): 235406-235415.
[11] Walther J H, Jaffe R, Halicioglu T, et al. Carbon nanotubes in water: Structural characteristics and energetics [J]. Journal of Physical Chemistry B, 2001,105(41): 9980-9987.
[12] Rappe A K, Casewit C J, Golwell K S, et al. Uff,a full periodic table force field for molecular mechanics and molecular dynamics simulations [J]. Journal of the American Chemical Society, 1992, 114(25): 10024-10035.
[13] Hess B, Carsten K, Lindahl E, et al. GROMACS 4: Algorithms for highly efficient, load-balanced, and scalable molecular simulation [J]. Journal of Chemical Theory and Computation, 2008, 4(3): 435-447.